The most interesting outcome of this smallness of \(\epsilon \)  is of course the enhancement of the
BEC mass \(m\)  from its `Hubble value' (\(m_{_H} \simeq 10^{-32}\)  eV)The Hubble value
is nothing but the one obtained by assuming the BEC constituents to be the gravitons, whence
taking the Gaussian spread \(\sigma \simeq H_{\text{\tiny 0}}^{-1}\)  one gets \(m \equiv m_{_H} \simeq 2\sqrt{2} H_{\text{\tiny 0}}\simeq 10^{-32}\)  eV, as \(H_{\text{\tiny 0}}\simeq 10^{-42}\)  GeV in the units \(c = 1 = \hbar \)  (see ref.
[1]})., since by Eq. (REF ), \(m\)  varies approximately as \(\epsilon ^{-1}\) .
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